37. f(x,y,z) = xyz, g(x,y,z) = x +2y + 3z = 6 => \lf = {yz,xz,xy) = >..Vg = (>.., 2>.,3>.). SECTION 14.8 LAGRANGE MULTIPLIERS D 233 Then >. = yz = ~xz = ~xy implies x = 2y, z = %Y· But 2y + 2y + 2y = 6 soy = 1, x = 2, z = ~ and the <strong>vol</strong>ume is V = ~- 39. f(x, y, z) = xyz, g(x, y ,.z) = 4(x + y + z) = c => \7 f = (yz, xz, x y), >.Vg = (4>., 4>., 4>.). Thus 4>. = yz = xz = xy or x = y = z = fie are the dimensions giving the maximum <strong>vol</strong>ume. 41 . If the dimensions of the box are given by x, y, and z, then we ne<strong>ed</strong> to find the maximum value of f(x, y, z) = xyz [x, y, z > 0) subject to the constraint L = ..jx 2 + y 2 + z 2 or g(x, y, z) = x 2 + y 2 + z 2 = £ 2 . \7 f = ).. \lg => yz xz (yz , xz, xy ) = >.(2x, 2y, 2z), so yz = 2>.x => >. = - , xz = 2>.y => >. = - , and xy = 2.Xz => 2 X 2 Y · Thus). = yz = xz .=> x 2 = y 2 [since z =f. 0) => x = y and >.= y 2 z = x 2 y. => x = z [since y =f. 0]. ~ ~ X Z Substituting into the constraint equation gives x 2 + x 2 + x 2 = L 2 => x 2 = £ 2 / 3 · => x = L / V3 = y = z and the maximum <strong>vol</strong>ume is (L/V3) 3 = £ 3 / (3 V3). 43. We ne<strong>ed</strong> to find the extreme values of f(x, y, z) = x 2 + y 2 + z 2 subject to the two constraints g(x, y , z) = x + y + 2z = 2 and h(x, y, z) = x 2 + y~ - z = 0. \lf = ( ~x , 2y, 2z}, >. \lg = (>., >., 2>.) and ~\l h = (2J.Lx_, 2~y , - ~ ). Thus we ne<strong>ed</strong> 2x = ). + 2J.LX (1), 2y = >. + 2~y (2), 2z = 2>.- f.t (3), x + y + 2z = 2 (4), and x 2 + y 2 - z = 0 (5). From (l) and (2), 2(x - y) = 2 ~ (x - y), so if x =f. y, ~ = 1. Putting this in (3) give,s 2z = 2>.- 1 or >. = z +~. bu t p ~1ttin g ~ = 1 into (l) says>. = 0. Hence z + ~ = 0 or z = -~. Then (4) and (5) become x + y- 3 = 0 and x 2 + y 2 + ~ ~ 0. The · last equation cannot be true, so this case gives no solution. So we must have x = y. Then (4) and (5) become 2x + 2z = 2 and 2x 2 - z = 0 which imply z = 1 - x and z = 2x 2 . Thus 2x 2 = 1 - x or 2x 2 + x - 1 = (2x - 1)(x + 1) = 0 s o x= ~ or x = - 1. The two points to check are (t, ~ . ~)and ( - 1, - 1, 2): /(~. ~. ~) = ~and f(-1, -1, 2) = 6. Thus(~,~. ~) is the point on the ellipse nearest the origin and ( - 1, - 1, 2) is the one farthest from the origin. 45. f(x, y , z) = yex-::, g(x, y, z) = 9x 2 + 4y 2 + 36z 2 = 36, h(x, y , z) = xy + yz = 1. \7 f = >.Vg + J-L\lh => (yex-::, ex - z, - yex- z) = >.(18x, 8y, 72z) + i'(V, x + z, y), so yex-z = 18>.x + J.l.V, ex- z = 8>.y + ~(x + z), - yex- :: = 72>.z + ~y . 9x 2 + 4y 2 + 36z 2 .= 36, x y + yz = 1. Using a CAS to solve these 5 equations simultaneously for x, y, z , >. , and ~ (in Maple, use the all values command), we get 4 real-yalu<strong>ed</strong> solutions: X~ 0.222444, y ~ · -2.157012, z ~ - 0.686049, >. ~ - 0.200401, ~ ~ 2.108584 X~ - 1.951921, y ~ - 0.545867, z ~ 0.119973, ). ~ 0.003141, ~ ~ - 0.076238 X ~ 0.155142, y ~ 0.904622, z ~ 0.950293, >. ~ - 0.012447, f.' ~ 0.489938 X~ 1.138731, y ~ 1.768057, . z ~ -0.573138, >. ~ 0.317141, f.' ~ 1.862675 Substituting these values into f gives /(0.222444, -2.157012, - 0.686049) ~ -5.3506, ® 20 12 Ceng3gc (.earning.. All Righrs Re~ r\'\,.-d. May not be scann<strong>ed</strong>, copi<strong>ed</strong>, or duplicat<strong>ed</strong>, or post<strong>ed</strong> to u publicly acct"Ssibh.: website, in whole or in 1.1r1 .
234 0 CHAPTER 14 PARTIAL DERIVATIVES f( -1.951921, - 0.545867, 0.119973) ~ -0.0688, !(0.155142, 0.904622, 0.950293) ~ 0.4084, !(1.138731, 1.768057, -0.573138) ~ 9.7938. Thus the maximum is approximately 9.7938, and the minimum is approximately -5.3506. 47. (a) We wish to maximize j(x1, x2, ... , xn) = ytx1x2 · · · Xn subject to g(x1,x2, .. . , Xn) = X1 +x2 + · · · +xn = c and X.;> 0. \1 f = ( ~ (X!X2 · .. Xn).; -l(X2 .. · Xn) , ~(X1X2 .. · Xn)'~-l (X!X3 · .. Xn), ... , ~(X t X2 · .. Xn) -!,-l (xl · .. Xn-1) ~ and >. V g = (>., >., ... , >.),so we ne<strong>ed</strong> to solve the system of equations 1/n 1/n 1/n , x 1 x 2 · · · Xn = nAx1 1 ( ).l.-1( ;;: XtX2 · • • Xn " XtX3 • · • Xn) = A 1/n 1/n 1/n \ X 1 X 2 · · · Xn = nAX2 This implies n>.x1 = n>.x2 = · · · = n>.x ... Note >. =I 0, otherwise we can't have all x.; > 0. Thus X1 = x2 -= · · · = Xn. But X ! + X2 + · · · + Xn = c => nx1 = c => X1 = ~ = X2 = X3 = · · · = Xn - Then the only point where f can n have an extreme value is (~ , ~, ... , ~). Since we can choose yalues for ( Xt, x2, ... , Xn) that make f as close to n n n zero (but not equal) as we like, f has no minimum value. Thus the maximum value is t(;,;, .... ;) = \};-; ..... ;=;. (b) From part (a), ~ i s the maximum value of f. Thus j(x1; x2, . .. , x n ) = ytx1x2 · · · Xn :::; ~- n ,-,-,---,------~· -- X1 + X2 + ··• + Xn . . x 1 + x2 + ··· + Xn = c, so ytx1X2 · · · Xn :::; n n But . These two means are equal when f attams 1ts maximum value ~' but this can occur only at the point(;,*' . .. , * ) we found in part (a). So the means are equal only - c when Xt = X2 = X3 = · · · = Xn = -. - n 14 Review CONCEPT CHECK 1. (a) A function f of two variables is a rule that assigns to each order<strong>ed</strong> pair (x, y) of real numbers in its domain a unique real number denot<strong>ed</strong> by f(x, y). (b) One way to visualize a function of two variables is by graphing it, resulting in the surface z = f(x, y). Another method for visualizing a function of two variables is a contour map. The contour map consists of level curves ofthe function which are horizontal traces of the graph of the function project<strong>ed</strong> onto the xy-plane. Also, we can use an arrow diagram such as Figure I in Section 14.1. © 2012 Cengage Le'ilming. All Rights Reserv<strong>ed</strong>. May nor be scnnncd. copi<strong>ed</strong>. or duplicntc:d, or postr..'tl ton publicly accessible wch~itc, in whole or in part.
- Page 1 and 2:
- STUDENT SOLUTIONS MANUAL for STEW
- Page 3 and 4:
.. BROOKS/COLE ~ I ~~r CENGAGE Lear
- Page 5 and 6:
D ABBREVIATIONS AND SYMBOLS CD cu D
- Page 7 and 8:
viii o CONTENTS 12.4 The Cross Prod
- Page 9 and 10:
10 D PARAMETRIC EQUATIONS AND POLAR
- Page 11 and 12:
SECTION 10.1 CURVES DEFINED BY PARA
- Page 13 and 14:
SECTION 10.1 CURVES DEFINED BY PARA
- Page 15 and 16:
SECTION 10.2 CALCULUS WITH PARAMETR
- Page 17 and 18:
SECTION 10.2 CALCULUS WITH PARAMETR
- Page 19 and 20:
SECTION 10.2 CALCULUS WITH PARAMETR
- Page 21 and 22:
SECTION 10.3 POLAR COORDINATES 0 13
- Page 23 and 24:
SECTION 10.3 POLAR COORDINATES 0 15
- Page 25 and 26:
SECTION 10.3 POLAR COORDINATES 0 17
- Page 27 and 28:
SECTION 10 .~ POLAR COORDINATES 0 1
- Page 29 and 30:
SECTION 10.4 A~~S AND LENGTHS IN PO
- Page 31 and 32:
SECTION 10.4 AREAS AND LENGTHS IN P
- Page 33 and 34:
SECTION 10.4 AREAS AND LENGTHS IN P
- Page 35 and 36:
SECTION 10.5 CONIC SECTIONS 0 27 5.
- Page 37 and 38:
SECTION 10.5 CONIC SECTIONS 0 29 35
- Page 39 and 40:
x2 y2 y2 a:2 _ a2 b 61. ;_2 - - = 1
- Page 41 and 42:
SECTION 10.6 CONIC SECTIONS IN POLA
- Page 43 and 44:
CHAPTER 10 REVIEW 0 35 the length o
- Page 45 and 46:
CHAPTER 10 REVIEW 0 37 EXERCISES 1.
- Page 47 and 48:
CHAPTER 10 REVIEW 0 39 25. x = t +
- Page 49 and 50:
CHAPTER 10 REVIEW 0 41 2 2 . 45. ~
- Page 51 and 52:
0 PROBLEMS PLUS l lt sin u dx cost
- Page 53 and 54:
11 . D INFINITE SEQUENCES AND SERIE
- Page 55 and 56:
SECTION 11.1 SEQUENCES 0 47 35. a,.
- Page 57 and 58:
SECTION 11.1 SEQUENCES D 49 71. Sin
- Page 59 and 60:
SECTION 11.2 SERIES 0 51 ak+l- a1.:
- Page 61 and 62:
SECTION 11.2 SERIES 0 53 13. n s.,
- Page 63 and 64:
SECTION 11.2 SERIES 0 55 47. F~r th
- Page 65 and 66:
. . (1+ c)- 2 scn es and set 1t equ
- Page 67 and 68:
SECTION 11.3 THE INTEGRAL TEST AND
- Page 69 and 70:
, SECTION 11.3 THE INTEGRAL TEST AN
- Page 71 and 72:
SECTION 11.4 THE COMPARISON TESTS D
- Page 73 and 74:
SECTION 11.5 ALTERNATING SERIES 0 6
- Page 75 and 76:
SECTION 11.5 ALTERNATING SERIES D 6
- Page 77 and 78:
SECTION 11.6 ABSOLUTE CONVERGENCE A
- Page 79 and 80:
SECTION 11.6 ABSOLUTE CONVERGENCE A
- Page 81 and 82:
17 lim I an+l I= SECTION 11.7 STRAT
- Page 83 and 84:
SECTION 11.8 POWER SERIES 0 75 l 00
- Page 85 and 86:
SECTION 11.8 POWER SERIES 0 n (b) I
- Page 87 and 88:
SECTION 11.9 REPRESENTATIONS OF FUN
- Page 89 and 90:
SECTION 11.9 REPRESENTATIONS OF FUN
- Page 91 and 92:
SECTION 11.10 TAYLOR AND MACLAURIN
- Page 93 and 94:
SECTION 11.10 TAYLOR AND MACLAURIN
- Page 95 and 96:
SECTION 11.10 TAYLOR AND MACLAURIN
- Page 97 and 98:
61 _ x_ x · sin x - x- tx 3 + 1~
- Page 99 and 100:
SECTION 11.11 APPLICATIONS OF TAYLO
- Page 101 and 102:
SECTION 11.11 APPLICATIONS OF TAYLO
- Page 103 and 104:
SECTION 11.11 APPLICATIONS OF TAYLO
- Page 105 and 106:
CHAPTER 11 REVIEW 0 97 J'(xn)(xn -
- Page 107 and 108:
CHAPTER 11 REVIEW 0 99 oo f (n) (O)
- Page 109 and 110:
CHAPTER 11 REVIEW 0 101 l 23. Consi
- Page 111 and 112:
49./- 1 - dx = -ln{4- x) + C and 4-
- Page 113 and 114:
D PROBLEMS PLUS 1. It would be far
- Page 115 and 116:
CHAPTER 11 PROBLEMS PLUS D 107 l 9.
- Page 117 and 118:
CHAPTER 11 PROBLEMS PLUS 0 109 x x
- Page 119 and 120:
112 0 CHAPTER 12 VECTORS AND THE GE
- Page 121 and 122:
114 0 CHAPTER 12 VECTORS AND THE GE
- Page 123 and 124:
116 0 CHAPTER 12 VECTORS AND THE GE
- Page 125 and 126:
118 0 CHAPTER 12 VECTORS AND THE GE
- Page 127 and 128:
120 D CHAPTER 12 VECTORS AND THE GE
- Page 129 and 130:
122 0 CHAPTER 12 VECTORS AND THE GE
- Page 131 and 132:
124 0 CHAPTER 12 VECTORS AND THE GE
- Page 133 and 134:
126 0 CHAPTER 12 VECTORS AND THE GE
- Page 135 and 136:
128 D CHAPTER 12 VECTORS AND THE GE
- Page 137 and 138:
130 D CHAPTER 12 VECTORS AND THE GE
- Page 139 and 140:
132 D CHAPTER 12 VECTORS AND THE GE
- Page 141 and 142:
134 D CHAPTER 12 VECTORS AND THE GE
- Page 143 and 144:
136 D CHA~TER 12 VECTORS AND THE GE
- Page 145 and 146:
138 D CHAPTER 12 VECTORS AND THE GE
- Page 147 and 148:
140 D CHAPTER 12 VECTORS AND THE GE
- Page 149 and 150:
142 D CHAPTER 12 VECTORS AND THE GE
- Page 151 and 152:
144 0 CHAPTER 12 VECTORS AND THE GE
- Page 153 and 154:
D PROBLEMS PLUS 1. Since three-dime
- Page 155 and 156:
l CHAPTER 12 PROBLEMS PLUS 0 149 Eq
- Page 157 and 158:
13 D VECTOR FUNCTIONS 13.1 Vector F
- Page 159 and 160:
SECTION 13.1 VECTOR FUNCTIONS AND S
- Page 161 and 162:
SECTION 13.1 VECTOR FUNCTIONS AND S
- Page 163 and 164:
SECTION 13.2 DERIVATIVES AND INTEGR
- Page 165 and 166:
SECTION 13.2 DERIVATIVES AND INTEGR
- Page 167 and 168:
SECTION 13.3 ARC LENGTH AND CURVATU
- Page 169 and 170:
SECTION 13.3 ARC LENGTH AND CURVATU
- Page 171 and 172:
SECTION 13.3 ARC LENGTH AND CURVATU
- Page 173 and 174:
SECTION 13.3 ARC LENGTH AND CURVATU
- Page 175 and 176:
SECTION 13.4 MOTION IN SPACE: VELOC
- Page 177 and 178:
2 SECTION 13.4 MOTION IN SPACE: VEL
- Page 179 and 180:
CHAPTER 13 REVIEW D 173 43. The tan
- Page 181 and 182:
5. f~(t 2 i +tcos 1rtj +sin 1rt k )
- Page 183 and 184:
CHAPTER 13 REVIEW 0 177 23. (a) r (
- Page 185 and 186:
180 0 CHAPTER 13 PROBLEMS PLUS (-2a
- Page 187 and 188: 182 0 CHAPTER 13 PROBLEMS PLUS vect
- Page 189 and 190: 184 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 191 and 192: 186 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 193 and 194: 188 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 195 and 196: 190 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 197 and 198: 192 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 199 and 200: 194 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 201 and 202: 196 D CHAPTER 14 PARTIAL DERIVATIVE
- Page 203 and 204: 198 D CHAPTER 14 PARTIAL DERIVATIVE
- Page 205 and 206: 200 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 207 and 208: 202 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 209 and 210: 204 D CHAPTER 14 PARTIAL DERIVATIVE
- Page 211 and 212: 206 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 213 and 214: 208 D CHAPTER 14 PARTIAL DERIVATIVE
- Page 215 and 216: 210 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 217 and 218: 212 D CHAPTER 14 PARTIAL DERIVATIVE
- Page 219 and 220: 214 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 221 and 222: 216 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 223 and 224: 218 D CHAPTER 14 PARTIAL DERIVATIVE
- Page 225 and 226: 220 D CHAPTER 14 PARTIAL DERIVATIVE
- Page 227 and 228: 222 D CHAPTER 14 PARTIAL DERIVATIVE
- Page 229 and 230: 224 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 231 and 232: 226 D CHAPTER 14 PARTIAL DERIVATIVE
- Page 233 and 234: 228 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 235 and 236: 230 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 237: 232 D CHAPTER 14 PARTIAL DERIVATIVE
- Page 241 and 242: 236 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 243 and 244: 238 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 245 and 246: 240 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 247 and 248: 242 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 249 and 250: D PROBLEMS PLUS 1. The areas of the
- Page 251 and 252: 15 D MULTIPLE INTEGRALS 15.1 Double
- Page 253 and 254: SECTION 15.2 ITERATED INTEGRALS D 2
- Page 255 and 256: l SECTION 15.3 DOUBLE INTEGRALS OVE
- Page 257 and 258: SECTION 15.3 DOUBLE INTEGRALS OVER
- Page 259 and 260: SECTION 15.3 DOUBLE INTEGRALS OVER
- Page 261 and 262: 61 . Since m :S j(x, y) :S M, ffD m
- Page 263 and 264: SECTION 15.4 DOUBLE INTEGRALS IN PO
- Page 265 and 266: SECTION 15.5 APPLICATIONS OF DOUBLE
- Page 267 and 268: SECTION 15.5 APPLICATIONS OF DOUBLE
- Page 269 and 270: SECTION 1505 APPLICATIONS OF DOUBLE
- Page 271 and 272: -I SECTION 15.6 SURFACE AREA 0 267
- Page 273 and 274: SECTION 15.7 TRIPLE INTEGRALS 0 269
- Page 275 and 276: SECTION 15.7 TRIPLE INTEGRALS D 271
- Page 277 and 278: Therefore E = { (x, y, z) I -2 ~ X~
- Page 279 and 280: 43. I,. = foL foL foL k(y2 + z2)dz.
- Page 281 and 282: SECTION 15.8 TRIPLE INTEGRALS IN CY
- Page 283 and 284: M xv = I~1f I: I:2 6 - 3 r 2 (zK) r
- Page 285 and 286: SECTION 15.9 TRIPLE INTEGRALS IN SP
- Page 287 and 288: SECTION 15.9 TRIPLE INTEGRALS IN SP
- Page 289 and 290:
(b) The wedge in question is the sh
- Page 291 and 292:
SECTION 15.10 CHANGE OF VARIABLES I
- Page 293 and 294:
CHAPTER 15 REVIEW 0 289 15 Review C
- Page 295 and 296:
CHAPTER 15 REVIEW 0 291 l 9. The vo
- Page 297 and 298:
CHAPTER 15 REVIEW D 293 33. Using t
- Page 299 and 300:
49. Since u = x- y and v = x + y, x
- Page 301 and 302:
298 D CHAPTER 15 PROBLEMS PLUS To e
- Page 303 and 304:
300 0 CHAPTER 15 PROBLEMS PLUS 13.
- Page 305 and 306:
16 0 VECTOR CALCULUS 16.1 Vector Fi
- Page 307 and 308:
SECTION 16.2 LINE INTEGRALS 0 305 2
- Page 309 and 310:
SECTION 16.2 LINE INTEGRALS 0 307 (
- Page 311 and 312:
SECTION 16.2 LINE INTEGRALS D 309 3
- Page 313 and 314:
SECTION 16.3 THE FUNDAMENTAL THEORE
- Page 315 and 316:
SECTION 16.4 GREEN'S THEOREM D 313
- Page 317 and 318:
SECTION 16.4 GREEN'S THEOREM 0 315
- Page 319 and 320:
8 8 8 (b)clivF = 'V ·iF=- (x+yz) +
- Page 321 and 322:
SECTION 16.5 CURL AND DIVERGENCE 0
- Page 323 and 324:
SECTION 16.6 PARAMETRIC SURFACES AN
- Page 325 and 326:
SECTION 16.6 PARAMETRIC SURFACES AN
- Page 327 and 328:
SECTION 16.6 PARAMETRIC SURFACES AN
- Page 329 and 330:
that is, D = {( x, y) I x 2 + y 2 :
- Page 331 and 332:
SECTION 16.7 SURFACE INTEGRALS 0 32
- Page 333 and 334:
SECTION 16.7 SURFACE INTEGRALS 0 33
- Page 335 and 336:
SECTION 16.8 STOKES' THEOREM 0 333
- Page 337 and 338:
dS SECTION 16.9 THE DIVERGENCE THEO
- Page 339 and 340:
CHAPTER 16 REVIEW 0 337 27. JI 5 cu
- Page 341 and 342:
CHAPTER 16 REVIEW 0 339 TRUE-FALSE
- Page 343 and 344:
CHAPTER 16 REVIEW D 341 Alternate s
- Page 345 and 346:
344 0 CHAPTER 16 PROBLEMS PLUS Simi
- Page 347 and 348:
3.c6 0 CHAPTER 17 SECOND-ORDER DIFF
- Page 349 and 350:
348 0 CHAPTER 17 SECOND-ORDER DIFFE
- Page 351 and 352:
350 0 CHAPTER 17 SECOND-ORDER DIFFE
- Page 353 and 354:
352 D CHAPTER 17 SECOND-ORDER DIFFE
- Page 355 and 356:
354 0 CHAPTER 17 SECOND-ORDER DIFFE
- Page 357 and 358:
356 D CHAPTER 17 SECOND-ORDER DIFFE
- Page 359 and 360:
0 APPENDIX Appendix H Complex Numbe
- Page 361:
APPENDIX H COMPLEX NUMBERS 0 361 43